Imaging optical system, imaging device, and imaging system

ABSTRACT

An imaging optical system is an optical system having an image circle formed on an imaging element. The imaging optical system includes: a plurality of lens elements arranged from an object side to an image plane side, and a diaphragm arranged between the plurality of lens elements. The plurality of lens elements includes a freeform lens having a freeform surface that is asymmetrical between a first direction and a second direction which cross with each other. At least two freeform lenses are located on the object side of the diaphragm.

BACKGROUND 1. Technical Field

The present disclosure relates to an imaging optical system, an imaging device, and an imaging system.

2. Related Art

WO 2003/010599 A discloses a method for capturing a panoramic image with a rectangular image sensor. In WO 2003/010599 A, a circular image is converted into a rectangular image by using a toric lens as a fisheye objective lens. Accordingly, in the rectangular image sensor, a rectangular image can be formed on a rectangular imaging element to capture a panoramic image.

SUMMARY

The present disclosure provides an imaging optical system, an imaging device, and an imaging system capable of facilitating to widen an angle of view in a specific direction.

An imaging optical system according to the present disclosure is an optical system having an image circle formed on an imaging element. The imaging optical system includes a plurality of lens elements arranged from an object side to an image plane side, and a diaphragm arranged between the plurality of lens elements. The plurality of lens elements includes a freeform lens having a freeform surface that is asymmetrical between a first direction and a second direction which cross with each other. At least two freeform lenses are located on the object side of the diaphragm.

An imaging device according to the present disclosure includes the imaging optical system described above and an imaging element. The imaging element captures an image formed by the imaging optical system. The imaging element has a first side which corresponds to the first direction and a second side which corresponds to the second direction and has a length equal to or shorter than the first side.

An imaging system according to the present disclosure includes the imaging device described above and an image processor. The image processor performs image processing on the image captured by the imaging element of the imaging device.

According to the imaging optical system, the imaging device, and the imaging system of the present disclosure, it is possible to facilitate to widen an angle of view in a specific direction.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a diagram showing a configuration of an imaging system according to a first embodiment of the present disclosure.

FIG. 2 is a diagram for describing an imaging element in the imaging system.

FIG. 3 is a lens layout diagram showing a configuration of an imaging optical system according to a first example.

FIG. 4 is a scatter plot showing the relationship between angle of view and image point in the imaging optical system according to a numerical example 1.

FIG. 5 is a diagram showing surface data of the imaging optical system according to the numerical example 1.

FIG. 6 is a diagram showing various kinds of data of the imaging optical system according to the numerical example 1.

FIG. 7 is a diagram showing freeform surface data of a third surface in the imaging optical system according to the numerical example 1.

FIG. 8 is a diagram showing freeform surface data of a fourth surface in the imaging optical system according to the numerical example 1.

FIG. 9 is a diagram showing freeform surface data of a fifth surface in the imaging optical system according to the numerical example 1.

FIG. 10 is a diagram showing freeform surface data of a sixth surface in the imaging optical system according to the numerical example 1.

FIG. 11 is a diagram showing aspherical surface data of a ninth surface in the imaging optical system according to the numerical example 1.

FIG. 12 is a diagram showing aspherical surface data of a tenth surface in the imaging optical system according to the numerical example 1.

FIG. 13 is a diagram showing freeform surface data of a fifteenth surface in the imaging optical system according to the numerical example 1.

FIG. 14 is a diagram showing freeform surface data of a sixteenth surface in the imaging optical system according to the numerical example 1.

FIG. 15 is an aberration diagram showing various aberrations of the imaging optical system according to the numerical example 1.

FIG. 16 is a chart showing the sufficiency of various conditions in the imaging optical system according to the first embodiment.

FIG. 17 is a diagram for describing various conditions in the imaging optical system.

FIG. 18 is a lens layout diagram showing a configuration of an imaging optical system according to a second example.

FIG. 19 is a diagram showing surface data of the imaging optical system according to a numerical example 2.

FIG. 20 is a diagram showing various kinds of data of the imaging optical system according to the numerical example 2.

FIG. 21 is a diagram showing freeform surface data of a second surface in the imaging optical system according to the numerical example 2.

FIG. 22 is a diagram showing freeform surface data of a third surface in the imaging optical system according to the numerical example 2.

FIG. 23 is a diagram showing freeform surface data of a fourth surface in the imaging optical system according to the numerical example 2.

FIG. 24 is a diagram showing freeform surface data of a fifth surface in the imaging optical system according to the numerical example 2.

FIG. 25 is a diagram showing freeform surface data of a sixth surface in the imaging optical system according to the numerical example 2.

FIG. 26 is a diagram showing aspherical surface data of a seventh surface in the imaging optical system according to the numerical example 2.

FIG. 27 is a diagram showing aspherical surface data of an eighth surface in the imaging optical system according to the numerical example 2.

FIG. 28 is a diagram showing freeform surface data of a thirteenth surface in the imaging optical system according to the numerical example 2.

FIG. 29 is a diagram showing freeform surface data of a fourteenth surface in the imaging optical system according to the numerical example 2.

FIG. 30 is a scatter plot showing the relationship between angle of view and image point in the imaging optical system according to the numerical example 2.

FIG. 31 is an aberration diagram showing various aberrations of the imaging optical system according to the numerical example 2.

FIG. 32 is a lens layout diagram showing a configuration of an imaging optical system according to a third example.

FIG. 33 is a diagram showing surface data of the imaging optical system according to a numerical example 3.

FIG. 34 is a diagram showing various kinds of data of the imaging optical system according to the numerical example 3.

FIG. 35 is a diagram showing aspherical surface data of a second surface in the imaging optical system according to the numerical example 3.

FIG. 36 is a diagram showing freeform surface data of a third surface in the imaging optical system according to the numerical example 3.

FIG. 37 is a diagram showing freeform surface data of a fourth surface in the imaging optical system according to the numerical example 3.

FIG. 38 is a diagram showing freeform surface data of a fifth surface in the imaging optical system according to the numerical example 3.

FIG. 39 is a diagram showing freeform surface data of a sixth surface in the imaging optical system according to the numerical example 3.

FIG. 40 is a diagram showing aspherical surface data of a fifteenth surface in the imaging optical system according to the numerical example 3.

FIG. 41 is a diagram showing freeform surface data of a seventeenth surface in the imaging optical system according to the numerical example 3.

FIG. 42 is a diagram showing freeform surface data of an eighteenth surface in the imaging optical system according to the numerical example 3.

FIG. 43 is a diagram showing freeform surface data of a nineteenth surface in the imaging optical system according to the numerical example 3.

FIG. 44 is a diagram showing freeform surface data of a twentieth surface in the imaging optical system according to the numerical example 3.

FIG. 45 is a scatter plot showing the relationship between angle of view and image point in the imaging optical system according to the numerical example 3.

FIG. 46 is an aberration diagram showing various aberrations of the imaging optical system according to the numerical example 3.

DESCRIPTION OF EMBODIMENTS

Hereinafter, the embodiments will be described in detail with reference to the drawings as appropriate. However, more detailed description than necessary may be omitted. For example, detailed descriptions of already well-known matters or duplicate descriptions of substantially the same configurations may be omitted. This is to avoid unnecessary redundancy in the following description and to facilitate understanding by those skilled in the art.

It should be noted that the applicant provides the accompanying drawings and the following description so that those skilled in the art can sufficiently understand the present disclosure, and they are not intended to limit the subject matter set forth in the claims.

First Embodiment

A first embodiment of an imaging optical system, an imaging device, and an imaging system according to the present disclosure will now be described with reference to the drawings.

1. Imaging System

The imaging system according to the present embodiment will be described with reference to FIG. 1. FIG. 1 is a diagram showing a configuration of an imaging system 10 according to the present embodiment.

As shown in FIG. 1, the imaging system 10 according to the present embodiment includes an imaging device 11 and an image processor 13, for example. The imaging device 11 includes an imaging optical system IL and an imaging element 12. The imaging device 11 is a device that captures images of various objects as subjects, such as various kinds of cameras. The image processor 13 may be incorporated in a camera or the like. Hereinafter, the direction of an optical axis D1 of the imaging optical system IL in the imaging device 11 is defined as a Z direction, the horizontal direction orthogonal to the Z direction is defined as an X direction, and the vertical direction orthogonal to the Z and X directions is defined as a Y direction.

The imaging optical system IL captures light that enters from the outside of the imaging device 11 and forms an image such as an image circle with the captured light. The imaging optical system IL is composed of a refractive optical system, for example. The imaging optical system IL will be described in detail later. Hereinafter, as shown in FIG. 1, the +Z side in the imaging optical system IL is defined as an image plane side, and the −Z side is defined as an object side.

The imaging element 12 is a CCD or CMOS image sensor, for example. The imaging element 12 has an imaging surface in which multiple pixels are two-dimensionally arranged at equal intervals. The imaging element 12 is disposed in the imaging device 11 such that the imaging surface is located on the image plane of the imaging optical system IL. The imaging element 12 captures an image formed on the imaging surface via the imaging optical system IL, to generate an image signal indicating the captured image.

The image processor 13 performs predetermined image processing on the image captured by the imaging device 11 on the basis of the image signal from the imaging element 12. The image processing is gamma correction and distortion correction, for example. The image processor 13 includes, for example, a CPU or MPU that implements various functions by executing a program stored in an internal memory. The image processor 13 may include a dedicated hardware circuit designed to achieve a desired function. The image processor 13 may include a CPU, MPU, GPU, DSP, FPGA, ASIC, or the like.

In the imaging system 10 according to the present embodiment, the imaging surface of the imaging element 12 is formed in a rectangular shape, for example. The imaging surface of the imaging element 12 will be described with reference to FIG. 2.

FIG. 2 shows a case where the imaging surface of the imaging element 12 is rectangular. The imaging element 12 has a long side Dx and a short side Dy that define the imaging surface. In the example of FIG. 2, the long side Dx is orthogonal to the short side Dy and is longer than the short side Dy. The imaging element 12 is disposed such that the long side Dx is parallel to the X direction and the short side Dy is parallel to the Y direction. Hereinafter, the X direction may be referred to as a long side direction, and the Y direction may be referred to as a long side direction.

FIG. 2 illustrates the positional relation between an image circle Is formed by the imaging optical system IL and the imaging surface. The image circle Is in the present embodiment has a shape distorted from a circular shape to an ellipse or the like, and has a major axis Ix and a minor axis Iy. In the example of FIG. 2, the major axis Ix is orthogonal to the minor axis Iy and is longer than the minor axis Iy. The imaging optical system IL is disposed so that the major axis Ix of the image circle Is is parallel to the X direction and the minor axis Iy is parallel to the Y direction so as to correspond to the long side Dx and the short side Dy of the imaging element 12. In the present embodiment, the X direction is an example of a first direction, and the Y direction is an example of a second direction. Further, the long side Dx is an example of a first side, and the short side Dy is an example of a second side.

The image circle Is of the imaging optical system IL has a portion that is not included in the range of the imaging surface of the imaging element 12, for example. In the example of FIG. 2, the major axis Ix of the image circle Is is longer than the long side Dx of the imaging element 12. The minor axis Iy of the image circle Is is longer than the short side Dy of the imaging element 12. The imaging element 12 captures an image by the image circle Is within the range of the imaging surface.

In the imaging system 10 as described above, the imaging optical system IL according to the present embodiment enables widening of an angle of view in the short side direction (i.e., the Y direction), as well as ensuring resolution of the captured image captured by the imaging element 12. The imaging optical system IL according to the present embodiment will be described below in detail.

2. Imaging Optical System

First to third examples of the imaging optical system IL will be described below each as an example in which the imaging optical system IL according to the present embodiment is concretely embodied.

2-1. First Example

An imaging optical system IL1 according to the first example will be described with reference to FIGS. 3 to 15.

FIG. 3 is a lens layout diagram showing a configuration of the imaging optical system IL1 according to the first example. The following lens layout diagrams show the arrangement of various lenses of the imaging optical system IL1 when focus is at infinity, for example. FIG. 3(a) is a lens layout diagram in a YZ cross-section of the imaging optical system IL1 according to the present example. FIG. 3(b) is a lens layout diagram in an XZ cross-section of the imaging optical system IL1. The YZ cross-section and the XZ cross-section are virtual cross-sections along an optical axis D1 of the imaging optical system IL1.

In FIG. 3(a), curved surfaces marked with “*” and “⋅” indicate freeform surfaces. The freeform surface is a rotationally asymmetric curved surface with respect to the optical axis D1. For example, the freeform surface marked with “*” is an XY-polynomial surface described later (see equation (E2)), and the freeform surface marked with “⋅” is an anamorphic aspherical surface described later (see equation (E1)). It should be noted that the symbols are omitted in FIG. 3(b).

The imaging optical system IL according to the present embodiment has multiple freeform surfaces that are asymmetric between the X direction and the Y direction, as shown in FIGS. 3(a) and 3(b), for example. Hereinafter, a lens element having a freeform surface on at least one of the object side and the image plane side is referred to as a freeform lens.

The imaging optical system IL1 according to the first example includes first to eighth lens elements L1 to L8 and a diaphragm A. As shown in FIG. 3(a), in the imaging optical system IL1, the first to eighth lens elements L1 to L8 are arranged in order from the object side to the image plane side along the optical axis D1. The diaphragm A is an aperture diaphragm.

In the imaging optical system IL1 according to the present example, the first lens element L1 located closest to the object side is a fisheye lens. The first lens element L1 of the present example is a spherical lens that is rotationally symmetric with reference to the optical axis D1. For example, the first lens element L1 has a negative meniscus shape, and is arranged with its convex surface facing the object side.

In the present example, the second lens element L2 is a freeform lens having freeform surfaces on both the object side and the image plane side. The third lens element L3 is a freeform lens having freeform surfaces on both sides. In the imaging optical system IL1 of the present example, according to the second and third lens elements L2 and L3, four freeform surfaces are provided on the object side of the diaphragm A, and two freeform lenses are adjacent to each other.

The fourth lens element L4 is a spherical lens having a negative meniscus shape, for example. The fourth lens element L4 is arranged with its convex surface facing the image plane side. The fifth lens element L5 is an aspheric lens, and has rotationally symmetric aspherical surfaces on both sides, for example. The fifth lens element L5 has a negative meniscus shape, and is arranged with its convex surface facing the image plane side, for example. The diaphragm A is arranged between the fifth lens element L5 and the sixth lens element L6.

The sixth lens element L6 is a spherical lens having a biconvex shape, for example. The sixth lens element L6 and the seventh lens element L7 are joined with each other, for example. The seventh lens element L7 is a spherical lens having a biconcave shape, for example. The eighth lens element L8 is a freeform lens having freeform surfaces on both sides, for example. In the imaging optical system IL1 according to the present example, the eighth lens element L8 provides a freeform surface on the image plane side of the diaphragm A.

In the imaging optical system IL1 configured as described above, the second and third lens elements L2 and L3, which are freeform lenses, are located on the object side of the diaphragm A. According to multiple freeform surfaces of the lens elements L2 and L3, light beams incident on the imaging optical system IL1 from the outside to condense at the diaphragm A can be controlled asymmetrically, and the angle of view in which the imaging optical system IL1 captures light can be widened in a specific direction such as the Y direction. Further, the imaging optical system IL1 can obtain an image in which the vicinity of the center is enlarged on the image plane by asymmetric control of the captured light beam. The effects of the imaging optical system IL1 described above will be described with reference to FIG. 4.

FIG. 4 is a scatter plot showing the relationship between angle of view and image point P1 in the imaging optical system IL1 according to the present example. In FIG. 4, image points P1 at which incident light forms an image on the image plane are plotted for each predetermined angular width in the entire angle of view of the imaging optical system IL1. The angular width is set to 10°. Further, the imaging optical system IL1 is set such that focus is at infinity.

The plots in FIG. 4 are based on a numerical example 1 in which the imaging optical system IL1 according to the first example is numerically implemented. The numerical example 1 of the imaging optical system IL1 will be described later. FIG. 4 shows image points P1 in the first quadrant on the XY plane of the image plane with the position of the optical axis D1 as an origin. Since the imaging optical system IL1 according to the present example is line-symmetric with respect to the X axis and the Y axis, plots in the second to fourth quadrants are similar to those in FIG. 4.

According to FIG. 4, despite the Y image height being shorter than the X image height, the number of image points P1 along the X axis and the number of image points P1 along the Y axis for each of the above angular widths are both ten in the imaging optical system IL1 according to the present example. Therefore, widening of an angle of view in the Y direction can be achieved. Further, in both the X direction and the Y direction, the distance between the image points P1 is greater as the image points P1 are closer to the origin. That is, it is possible to form an image in which a region within a predetermined range near the center is more enlarged than the end portion on the image plane.

From the relative perspective to the enlargement of the image at the center as described above, on the imaging surface of the imaging element 12, more pixels are allocated to the enlarged region near the center than to other regions. Therefore, the imaging device 11 according to the present embodiment can capture an image with higher resolution in the vicinity of the center with the angle of view ensured widely. As in FIG. 4, the change in the distance between the image points P1 is remarkable especially in the Y direction. As a result, the imaging device 11 according to the present embodiment can increase resolution near the center in the vertical direction as well as enabling capturing a wide range in the vertical direction.

The numerical example 1 corresponding to the imaging optical system IL1 according to the first example as described above will be described with reference to FIGS. 5 to 15.

FIG. 5 is a diagram showing surface data of the imaging optical system IL1 according to the numerical example 1. The surface data of FIG. 5 shows a surface type, and a radius of curvature r and distance d between adjacent surfaces in mm for each of surfaces s1 to s16 of the imaging optical system IL1 arranged in order from the object side, and a refractive index nd and an Abbe number vd to the d-line of each lens element. Surface types include spherical surfaces, aspherical surfaces, anamorphic surfaces, and XY-polynomial surfaces.

FIG. 6 is a diagram showing various kinds of data of the imaging optical system IL1 according to the numerical example 1. The various kinds of data in FIG. 6 show an F number, a vertical half angle of view, a horizontal half angle of view, a vertical image height, and a horizontal image height according to the present numerical example. The unit of image heights is “mm”, and the unit of half angles of view is “°”.

FIG. 7 is a diagram showing freeform surface data of the third surface s3 in the imaging optical system IL1 according to the numerical example 1. The freeform surface data of FIG. 7 shows various coefficients of the following equation (E1) that defines the anamorphic spherical surface as a freeform surface for the object-side surface of the second lens element L2.

$\begin{matrix} {\mspace{79mu} \left\lbrack {{Equation}\mspace{14mu} 1} \right\rbrack} & \; \\ {z = {\frac{{({CUX})x^{2}} + {({CUY})y^{2}}}{1 + \sqrt{1 - {({CUX})^{2}x^{2}} - {({CUY})^{2}y^{2}}}} + {{AR}\left\{ {{\left( {1 - {AP}} \right)x^{2}} + {\left( {1 + {AP}} \right)y^{2}}} \right\}^{2}} + {{BR}\left\{ {{\left( {1 - {BP}} \right)x^{2}} + {\left( {1 + {BP}} \right)y^{2}}} \right\}^{3}} + {{CR}\left\{ {{\left( {1 - {CP}} \right)x^{2}} + {\left( {1 + {CP}} \right)y^{2}}} \right\}^{4}} + {{DR}\left\{ {{\left( {1 - {DP}} \right)x^{2}} + {\left( {1 + {DP}} \right)y^{2}}} \right\rbrack^{5}}}} & \left( {E\; 1} \right) \end{matrix}$

In the above equation (E1), CUX, CUY, AR, AP, BR, BP, CR, CP, DR, and DP are coefficients. According to the above equation (E1), a sag amount z at the position of coordinates (x, y) on the target surface is determined. Here, the above equation (E1) has regularity that is based on coordinate variables x and y only in the form of a weighted sum in which x² and y² are weighted by the above coefficients. That is, the anamorphic aspherical surface is a freeform surface that is rotationally asymmetric under constraint of regularity of the equation (E1) described above.

FIG. 8 is a diagram showing freeform surface data of the fourth surface s4 in the imaging optical system IL1 according to the numerical example 1. The freeform surface data of FIG. 8 shows various coefficients of the XY polynomial defining the XY-polynomial surface as the freeform surface of the image-plane-side surface of the second lens element L2. The XY polynomial is expressed by the following equation (E2).

[Equation  2] $\begin{matrix} {{z = {\frac{{cr}^{2}}{1 + \sqrt{1 - {\left( {1 + K} \right)c^{2}r^{2}}}} + {\sum\limits_{j = 2}^{66}\; {c_{j}x^{p}y^{q}}}}}{j = {\frac{\left( {p + q} \right)^{2} + p + {3q}}{2} + 1}}} & ({E2}) \end{matrix}$

In the above equation (E2), c is a peak curvature, K is a conic constant, and c_(j) is a coefficient. In the second term on the right side of the above equation (E2), j is an integer of e.g. 2 or more and 66 or less, and the summation for each j is calculated. According to the above equation (E2), a sag amount z at the position of (x, y) coordinates on the target surface is determined more freely than the regularity of the anamorphic aspherical surface.

FIGS. 9 and 10 are diagrams respectively showing freeform surface data of the fifth surface s5 and the sixth surface s6 in the imaging optical system IL1 according to the numerical example 1. Similarly to FIG. 8, the freeform surface data in FIGS. 9 and 10 respectively show various coefficients of equation (E2) for the object-side surface and the image-plane-side surface of the third lens element L3.

FIGS. 11 and 12 are diagrams respectively showing aspherical surface data of the ninth surface s9 and the tenth surface s10 in the imaging optical system IL1 according to the numerical example 1. The aspherical surface data in FIGS. 11 and 12 shows various coefficients of the following equation (E3) that defines the shape of the aspherical surface for the object-side surface and the image-plane-side surface of the fifth lens element L5.

[Equation  3] $\begin{matrix} {z = {\frac{h^{2}\text{/}r}{1 + \sqrt{1 - {\left( {1 + \kappa} \right)\left( {h\text{/}r} \right)^{2}}}} + {\Sigma \; A_{n}h^{n}}}} & ({E3}) \end{matrix}$

In the above equation (E3), h is a height in the radial direction, K is a conic constant, and An is an n-th order aspheric coefficient. In the second term on the right side of the above equation (E3), n is e.g. an even number of 4 or more and 20 or less, and the summation for each n is calculated. According to the above equation (E3), a sag amount z at the height h in the radial direction on the target surface is determined in a rotational symmetric manner.

FIGS. 13 and 14 are diagrams respectively showing freeform surface data of the fifteenth surface s15 and the sixteenth surface s16 in the imaging optical system IL1 according to the numerical example 1. Similarly to FIG. 7, the freeform surface data in FIG. 13 indicates various coefficients of equation (E1) for the object-side surface of the eighth lens element L8. Similarly to FIG. 8, the freeform surface data in FIG. 14 indicates various coefficients of equation (E2) for the image-plane-side surface of the eighth lens element L8.

FIG. 15 is an aberration diagram showing various aberrations of the imaging optical system IL1 according to the present example. The following aberration diagrams indicate various longitudinal aberrations when focus is at infinity. FIG. 15(a) shows a spherical aberration “SA” in the imaging optical system IL1. FIGS. 15(b), 15(c), and 15(d) show astigmatism “AST-V” in the Y direction, astigmatism “AST-H” in the X direction, and astigmatism “AST-D” in the diagonal direction, respectively.

The horizontal axis of each of FIGS. 15(a) to 15(d) is expressed in mm. The vertical axis in FIG. 15(a) is based on the pupil height. FIG. 15(a) shows characteristic curves of spherical aberration with respect to the d-line, F-line and c-line. The vertical axes in FIGS. 15(b) to 15(d) are based on a half angle of view. FIGS. 15(b) to 15(d) respectively show characteristic curves of astigmatism with respect to the XZ or YZ cross-section which is along the X direction or the Y direction and the optical axis D1.

In the present embodiment, as shown in FIGS. 7 to 10, 13, and 14, for example, only even terms of x and y are used in each freeform surface. Thus, the diagonal aberration “AST-D” and the like are the same in all of the first to fourth quadrants.

2-2. Various Conditions

Various conditions satisfied by the imaging optical system IL according to the present embodiment will be described with reference to FIGS. 16 and 17 using the numerical example 1 of the imaging optical system IL1.

FIG. 16 is a chart showing the sufficiency of various conditions in the imaging optical system IL according to the present embodiment. The chart of FIG. 16 shows that the imaging optical system IL according to the present embodiment satisfies the following conditions (1) to (7) in each of numerical examples 1 to 3.

The condition (1) is that the freeform surfaces of all the freeform lenses located on the object side of the diaphragm A in the imaging optical system IL satisfy the following conditional expression (1). The freeform lenses located on the object side of the diaphragm A enables to easily set an asymmetric angle of view by controlling light beams incident on the imaging optical system IL from the outside to condense at the diaphragm A.

[Equation  4] $\begin{matrix} {\frac{\sum\limits_{k = 1}^{N}\; {\left( {{SS}_{k} - {SL}_{k}} \right) \times \Delta \; {nd}_{k}}}{YSH} < 0} & (1) \end{matrix}$

In the above equation (1), N is the total number of freeform surfaces located on the object side (i.e., −Z side) of the diaphragm A. k is a number that indicates each freeform surface located on the −Z side of the diaphragm A, and is an integer from 1 to N. Hereinafter, it is assumed that the number k is set in ascending order to the image plane side (i.e., +Z side), where the freeform surface located closest to the −Z side from among the total N freeform surfaces is represented as k=1.

The left side of the above equation (1) is the summation of difference (PS_(k)−PL_(k)) between PS_(k) and PL_(k) for each freeform surface of the freeform lenses located on the −Z side of the diaphragm A:

PS_(k)=SS_(k)×Δnd_(k),

PL_(k)=SL_(k)×Δnd_(k)

where SS_(k) is a sag amount at a height YSH, which is a reference, of a k-th freeform surface in the Y direction, and indicates a representative value of a sag amount on the k-th freeform surface on the short side. The height YSH is 50% of the shortest image height in the imaging optical system IL, and is e.g. ¼ of the minor axis Iy of the image circle Is in FIG. 2. SL_(k) is a representative value of a sag amount on the k-th freeform surface on the long side, and is a sag amount at the height YSH in the X direction. Δnd_(k) is a difference resulting from subtracting a refractive index on the −Z side of the k-th freeform surface from a refractive index on the +Z side of the k-th freeform surface.

PS_(k) indicates the tendency of power (i.e., refractive power) in the YZ cross-section of the lens according to the sag amount SS_(k) of the k-th freeform surface on the short side. PL_(k) indicates the tendency of power in the XZ cross-section according to the sag amount SL_(k) of the same freeform surface on the long side. PS_(k) and PL_(k) is described with reference to FIG. 17.

FIG. 17 illustrates the YZ cross-section of a lens element Lk having a k-th freeform surface on the −Z side and a (k+1)th freeform surface on the +Z side. FIG. 17 illustrates a case where the lens element Lk has a biconvex shape as a whole and produces positive power on both surfaces. In this case, the sag amount SS_(k) on the −Z side surface of the lens element Lk is positive as shown in FIG. 17. The refractive index on the +Z side of the same surface is a refractive index nk based on the material of the lens element Lk, and the refractive index on the −Z side is a refractive index n0 based on air or the like. Therefore, the difference Δnd_(k) between the refractive index nk on the +Z side and the refractive index n0 on the −Z side of this surface is positive, and PS_(k)=SS_(k)×Δnd_(k)>0 is established.

Further, the sag amount SS_(k+1) on the +Z side surface of the lens element Lk is negative as shown in FIG. 17. Thus, the difference Δnd_(k+1) between the refractive indexes n0 and nk on the −Z side and the +Z side of the same surface is negative, that is, has a sign opposite to the sign of ΔAnd_(k). Therefore, PS_(k+1)=SS_(k+1)×Δnd_(k+1)>0 is established.

As described above, the sign of PS_(k) corresponds to the sign of the power in the YZ cross-section regardless of whether the corresponding freeform surface is on the +Z side or on the −Z side of the lens element Lk. The same applies to the sign of PL_(k) on the XZ cross-section.

In the freeform surface, a difference between PS_(k) and PL_(k) occurs depending on the difference between the sag amount SS_(k) on the short side and the sag amount SL_(k) on the long side. When the difference (PS_(k)−PL_(k)) is negative, the corresponding freeform surface tends to increase the power negatively in the YZ cross-section rather than in the XZ cross-section of the lens element Lk, that is, on the short side rather than on the long side.

In view of the above, satisfying conditional expression (1) makes the freeform surfaces of the imaging optical system IL located on the −Z side of the diaphragm A to negatively increase the power on the short side rather than on the long side as a whole. Therefore, the angle of view on the short side can be widened in the imaging optical system IL according to the condition (1).

FIG. 16 shows the calculated values for the left side of conditional expression (1). In the imaging optical system IL1 shown in FIG. 3, the summation of the left side of conditional expression (1) is calculated within a range of N=4, that is within the range up to the +Z side surface of the third lens element L3, with the −Z side surface of the second lens element L2 defined as k=1. Regarding the condition (1), the calculated value “−0.0204” of the imaging optical system IL1 according to the first example is below the upper limit value “0” which is a value on the right side of the above conditional expression (1), as shown in FIG. 16.

If the calculated value is above the upper limit value of the condition (1), it would be difficult to widen the angle of view on the short side, or the size of the optical system would be increased. The imaging optical system IL1 according to the first example also satisfies the condition that the upper limit value of conditional expression (1) is decreased from “0” to “−0.01”. This condition is referred to as condition (1′) below. According to the condition (1′), the angle of view on the short side can be more easily widened, and the optical system can be downsized.

The condition (2) is defined by the following conditional expression (2) based on the summation for the freeform surfaces of the freeform lenses located on the object side of the diaphragm A, similarly to the condition (1).

Σ^(N) _(k=1){(SS _(k) −SL _(k))×Δnd _(k) }/CTL1<−0.0002  (2)

where CTL1 is the thickness of the first lens element L1 that is located closest to the −Z side in the imaging optical system IL. The summation of the left side of conditional expression (2) is calculated within the same range as conditional expression (1). FIG. 16 shows the calculated values of the left side of conditional expression (2).

Above the upper limit value of conditional expression (2), it may be difficult to control astigmatism, or the size of the optical system may be increased. In contrast to this, as in the calculated values shown in FIG. 16, the imaging optical system IL1 according to the first example is below the upper limit value of conditional expression (2) and satisfies the condition (2), for example. Further, the imaging optical system IL1 according to the first example also satisfies the condition that the upper limit value of conditional expression (2) is decreased to “−0.002”. This condition is referred to as condition (2′) below. According to the condition (2′), it is possible to facilitate to control the astigmatism of the imaging optical system IL1 and to downsize the optical system.

The condition (3) is defined by the following conditional expression (3) based on the summation for the freeform surfaces of the freeform lenses located on the object side of the diaphragm A, similarly to the condition (1).

Σ^(N) _(k=1){(SS _(k) −SL _(k))×Δnd _(k) }/CTF<−0.001  (3)

where CTF is the thickness of the freeform lens located closest to the −Z side in the imaging optical system IL, and is the thickness of e.g. the second lens element L2 in the imaging optical system IL1 according to the first example. The summation of the left side of conditional expression (3) is calculated within the same range as conditional expression (1). FIG. 16 shows the calculated values of the left side of conditional expression (3).

Above the upper limit value of conditional expression (3), it may be difficult to widen the angle of view on the short side, or the optical system may be increased in size. In contrast to this, the imaging optical system IL1 according to the first example satisfies the condition (3) as shown in FIG. 16, for example. Further, the imaging optical system IL1 according to the first example also satisfies the condition that the upper limit value of conditional expression (3) is decreased to “−0.01”. This condition is referred to as condition (3′) below. According to the condition (3′), it is possible to improve to widen the angle of view on the short side of the imaging optical system IL1 and to downsize the optical system.

Further, in the imaging optical system IL1 according to the first example, the sign of (SS_(k)−SL_(k)) is negative in all of the freeform surfaces of k=1 to N on the −Z side of the diaphragm A. According to the sign of (SS_(k)−SL_(k)) being the same in the freeform surfaces of k=1 to N, it is possible to gradually bend the incident light beam in the imaging optical system IL1 and suppress an occurrence of aberration.

The condition (4) is defined by the following conditional expression (4) based on the summation for both surfaces of the freeform lens located closest to the −Z side in the imaging optical system IL and the summation for both surfaces of the freeform lens located closest to the +Z side on the −Z side of the diaphragm A.

[Equation  5] $\begin{matrix} {{- 2.00} < \frac{\sum\limits_{i = 1}^{2}\; {\left( {{SS}_{i} - {SL}_{i}} \right) \times \Delta \; {nd}_{i}}}{\sum\limits_{n = 1}^{2}\; {\left( {{SS}_{n} - {SL}_{n}} \right) \times \Delta \; {nd}_{n}}} < 3.00} & (4) \end{matrix}$

where the summation of the numerator on the middle side of the above equation (4) is calculated for the −Z side surface and the +Z side surface of the freeform lens located closest to the −Z side, with each surface specified by i=1, 2. That is, SS_(i) is a sag amount at the height YSH in the Y direction of the surface designated by i in the freeform lens. Similarly, SL_(i) is a sag amount at the same height YSH in the X direction of the i-th surface of the same freeform lens. For example, in the imaging optical system IL1 according to the first example, SL_(i) and SS_(i) are defined on the surfaces of the second lens element L2. Note that, if the i-th surface is not a freeform surface, SS_(i)=SL_(i) is established due to rotational symmetry, which does not contribute to the above summation.

The summation of the denominator on the middle side of the above equation (4) is calculated for the −Z side surface and the +Z side surface of the freeform lens located closest to the +Z side on the −Z side of the diaphragm A, with each surface specified by n=1, 2. Similarly to the above, SSn and SL_(n) are sag amounts at the positions having the height YSH in the X and Y directions of the surface designated by n in the freeform lens. For example, in the first example, SL_(n) and SS_(n) are defined on the surfaces of the third lens element L3.

Regarding conditional expression (4), below the lower limit value, it may be difficult to control astigmatism, and above the upper limit value, it may be difficult to widen the angle of view on the short side. In contrast to this, the imaging optical system IL1 according to the first example satisfies the condition (4) as shown in FIG. 16, for example. Further, the imaging optical system IL1 according to the first example also satisfies the condition that the lower limit value of conditional expression (4) is increased to “0.00” and the upper limit value is decreased to “2.00”. This condition is referred to as condition (4′) below. According to the condition (4′), it is possible to improve to control the astigmatism of the imaging optical system IL1 and widen the angle of view on the short side.

The condition (5) is defined by conditional expression (5) below, regarding the freeform surface located closest to the −Z side and the freeform surface located closest to the +Z side on the −Z side of the diaphragm A in the imaging optical system IL.

[Equation  6] $\begin{matrix} {{- 8.00} < \frac{\left( {{SS}_{1} - {SL}_{1}} \right) \times \Delta \; {nd}_{1}}{\left( {{SS}_{N} - {SL}_{N}} \right) \times \Delta \; {nd}_{N}} < 0.00} & (5) \end{matrix}$

where SL₁ and SS₁ are sag amounts at the height YSH in the X and Y directions of the freeform surface located closest to the −Z side. SL_(N) and SS_(N) are sag amounts at the height YSH in the X and Y directions of the freeform surface located closest to the +Z side on the −Z side of the diaphragm A. In the imaging optical system IL1 according to the first example, SL₁ and SS₁ are defined on the −Z side surface of the second lens element L2, and SL_(N) and SS_(N) are defined on the +Z side surface of the third lens element L3.

Regarding conditional expression (5), below the lower limit value, the optical system may be increased in size, and above the upper limit value, it may be difficult to widen the angle of view on the short side. In contrast to this, the imaging optical system IL1 according to the first example satisfies the condition (5) according to the calculated value shown in FIG. 16, for example. Further, the imaging optical system IL1 according to the first example also satisfies the condition that the lower limit value of conditional expression (5) is increased to “−6.00” and the upper limit value is decreased to “−2.00”. This condition is referred to as condition (5′) below. According to the condition (5′), it is possible to more downsize the imaging optical system IL1 and to more easily widen the angle of view on the short side.

Conditional expression (6) is defined by the following conditional expression (6) regarding refractive indexes of the freeform lenses located on the −Z side of the diaphragm A of the imaging optical system IL.

1≤nd1/ndN<1.3  (6)

where nd1 is the refractive index to the d-line of the freeform lens located closest to the −Z side. ndN is the refractive index to the d-line of the freeform lens located closest to the +Z side on the −Z side of the diaphragm A. For example, in the first example, nd1 is the refractive index of the second lens element L2, and ndN is the refractive index of the third lens element L3.

Regarding conditional expression (6), below the lower limit value, it may be difficult to control astigmatism, and above the upper limit value, it may be difficult to control the lateral chromatic aberration. In contrast to this, the imaging optical system IL1 according to the first example satisfies the condition (6) according to the calculated value shown in FIG. 16, for example. Thus, a situation in which it becomes difficult to control astigmatism and lateral chromatic aberration can be avoided.

Conditional expression (7) is defined by the following conditional expression (7), regarding the refractive index ndN of the freeform lens of the freeform lens located closest to the +Z side on the −Z side of the diaphragm A.

1.45<ndN<1.80  (7)

Regarding conditional expression (7), below the lower limit value, it may be difficult to control curvature of field, and above the upper limit value, it may be difficult to control the lateral chromatic aberration. In contrast to this, the imaging optical system IL1 according to the first example satisfies the condition (7) according to the calculated value shown in FIG. 16, for example. Further, the imaging optical system IL1 according to the first example also satisfies the condition that the lower limit value of conditional expression (7) is increased to “1.50” and the upper limit value is decreased to “1.60”. This condition is referred to as condition (7′) below. According to the condition (7′), it is possible to improve to control the curvature of field and the lateral chromatic aberration.

The imaging optical system IL according to the present embodiment is not limited to the imaging optical system IL1 in the first example described above, and can be implemented in various forms. For example, in the imaging optical system IL1 according to the first example, there are two freeform lenses located on the object side of the diaphragm A. However, in the imaging optical system IL according to the present embodiment, there may be three or more freeform lenses located on the object side of the diaphragm A.

2-3. Second Example

The second example describes an example of the imaging optical system IL in which there are three freeform lenses located on the object side of the diaphragm A. An imaging optical system IL2 according to the second example will be described with reference to FIGS. 18 to 31.

FIG. 18 shows the configuration of the imaging optical system IL2 according to the second example. FIGS. 18(a) and 18(b) are diagrams showing lens arrangement of the imaging optical system IL2, similarly to FIGS. 3(a) and 3(b).

The imaging optical system IL2 according to the second example includes first to seventh lens elements L1 to L7, which are sequentially arranged as in the first example, and a diaphragm A located between the fourth and fifth lens elements L4 and L5. In the imaging optical system IL2 according to the present example, the first lens element L1 is a freeform lens having an XY-polynomial surface on the image plane side. Further, the second and third lens elements L2 and L3 are freeform lenses having XY-polynomial surfaces on both sides.

In the present example, the first to third lens elements L1 to L3 as described above provide a total of five (N=5) freeform surfaces on the object side of the diaphragm A, with three freeform lenses being adjacent to each other. The sign of (SS_(k)−SL_(k)) on each freeform surface of k=1 to 5 on the object side of the diaphragm A is positive in the present example. Further, the seventh lens element L7, which is located closest to the image plane side, is a freeform lens having XY-polynomial surfaces on both sides. FIGS. 19 to 29 show a numerical example corresponding to the imaging optical system IL2 according to the second example.

FIG. 19 is a diagram showing surface data of the imaging optical system IL2 according to a numerical example 2. FIG. 20 is a diagram showing various kinds of data of the imaging optical system IL2 according to the present example. FIGS. 19 and 20 show the respective data as in FIGS. 5 and 6 according to the numerical example 1.

FIGS. 21 to 25 are diagrams respectively showing freeform surface data of second to sixth surfaces s2 to s6 in the imaging optical system IL2 according to the present example. Similarly to the numerical example 1, the freeform surface data in FIG. 21 indicates various coefficients of equation (E2) for the image-plane-side surface of the first lens element L1. Similarly, FIGS. 22 to 25 show freeform surface data on both surfaces of the second and third lens element L2 and L3.

FIGS. 26 and 27 show aspherical surface data of seventh and eighth surfaces s7 and s8 in the imaging optical system IL2 according to the present example, similarly to FIGS. 11 and 12. FIGS. 28 and 29 show freeform surface data of thirteenth and fourteenth surfaces s13 and s14 in the imaging optical system IL2, similarly to FIG. 14 and the like.

Based on the numerical example 2 described above, FIG. 30 shows the relationship between angle of view and image point P2 in the imaging optical system IL2 according to the present example. As shown in FIG. 30, according to the imaging optical system IL2 of the present example, an angle of view in the Y direction can also be widened as in the first example.

FIG. 31 shows various aberrations of the imaging optical system IL2 according to the present example. Similarly to FIGS. 15(a) to 15(d), FIGS. 31(a), 31(b), 31(c), and 31(d) are aberration diagrams of the imaging optical system IL2 according to the present example.

Further, the imaging optical system IL2 according to the present example satisfies the abovementioned conditions (1) to (7) as shown in FIG. 16. Further, the imaging optical system IL2 according to the present example also satisfies the condition that the lower limit value of conditional expression (6) is increased to “1.05” and the upper limit value is decreased to “1.2”. This condition is referred to as condition (6′) below. According to the condition (6′), it is possible to more easily control the astigmatism and the lateral chromatic aberration of the imaging optical system IL2.

2-4. Third Example

An imaging optical system IL3 according to the third example will be described with reference to FIGS. 32 to 46.

FIG. 32 shows the configuration of the imaging optical system IL3 according to the third example. FIGS. 32(a) and 32(b) are diagrams showing lens arrangement of the imaging optical system IL3, similarly to FIGS. 3(a) and 3(b).

The imaging optical system IL3 according to the third example includes first to tenth lens elements L1 to L10, which are sequentially arranged as in the first example, and a diaphragm A located between the fifth and sixth lens elements L5 and L6. In the imaging optical system IL3 in the present example, the first lens element L1 located closest to the object side is not a fisheye lens as in the first example, but has a biconcave shape. For example, the first lens element L1 is a rotationally symmetric aspheric lens having an aspherical surface on the image plane side.

In the present example, the second and third lens elements L2 and L3 are freeform lenses having freeform surfaces on both sides as shown in FIG. 32(a).

The fourth lens element L4 is a spherical lens having a biconvex shape. The fifth lens element L5 is a spherical lens having a positive meniscus shape, and is arranged with its convex surface facing the object side. The sixth lens element L6 is a spherical lens having a biconvex shape, and is joined with the seventh lens element L7. The seventh lens element L7 is a spherical lens having a biconcave shape. The eighth lens element L8 is an aspherical lens having an aspherical surface on the object side.

In the present example, the ninth lens element L9 is a freeform lens having freeform surfaces on both sides. Further, the tenth lens element L10 is a freeform lens having freeform surfaces on both sides. FIGS. 33 to 44 show a numerical example corresponding to the imaging optical system IL3 according to the third example.

FIG. 33 is a diagram showing surface data of the imaging optical system IL3 according to a numerical example 3. FIG. 34 is a diagram showing various kinds of data of the imaging optical system IL3 according to the present example. FIGS. 33 and 34 show the respective data as in FIGS. 5 and 6 according to the numerical example 1.

FIG. 35 is a diagram showing aspherical surface data of a second surface s2 in the imaging optical system IL3 according to the present example. Similarly to the numerical example 1, the aspherical surface data in FIG. 35 indicates various coefficients of equation (E3) for the image-plane-side surface of the first lens element L1.

FIGS. 36 to 39 are diagrams respectively showing freeform surface data of third to sixth surfaces s3 to s6 in the imaging optical system IL3 according to the present example. Similarly to the numerical example 1, FIGS. 36 to 39 show various coefficients of equation (E2).

FIG. 40 shows aspherical surface data of a fifteenth surface s15 in the imaging optical system IL3 according to the present example, similarly to FIG. 35. FIGS. 41 to 44 are diagrams respectively showing freeform surface data of seventeenth to twentieth surfaces s17 to s20 in the imaging optical system IL3. FIGS. 41 to 44 show each freeform surface data on both surfaces of the ninth and tenth lens elements L9 and L10, similarly to FIGS. 36 to 39.

Based on the numerical example 3 described above, FIG. 45 shows the relationship between angle of view and image point P3 in the imaging optical system IL3 according to the present example. FIG. 46 shows various aberrations of the imaging optical system IL3 in the present example. Similarly to FIGS. 15(a) to 15(d), FIGS. 46(a), 46(b), 46(c), and 46(d) are aberration diagrams of the imaging optical system IL3 according to the present example. The imaging optical system IL3 according to the present example satisfies the abovementioned conditions (1) to (7) as shown in FIG. 16. As described above, according to the imaging optical system IL3 of the present example, an angle of view in the short side direction can also be easily widened as in the first example.

Other Embodiments

The first embodiment has been described as an example of the technique disclosed in the present application. However, the technique in the present disclosure is not limited to the above embodiment, and is also applicable to other embodiments including appropriate modifications, substitutions, additions, or omissions. In addition, a new embodiment can be made by combining constituents described in the above embodiments. Accordingly, some other embodiments will be described below.

In the first embodiment described above, a rectangular imaging surface is illustrated in FIG. 2, but the imaging surface of the imaging element 12 is not limited thereto. In the present embodiment, the imaging surface of the imaging element 12 may have various quadrilateral shapes other than the rectangular shape, or may be partially masked. Further, the imaging surface of the imaging element 12 may be curved. With respect to the imaging element 12 described above, the same effect as that of the first embodiment can be obtained by the imaging optical system IL according to the present embodiment.

For example, the long side Dx and the short side Dy of the imaging element 12 of the present embodiment do not need to be orthogonal to each other, and may cross at various angles. Further, the imaging element 12 may have two sides having the same length instead of the long side Dx and the short side Dy. In the imaging optical system IL according to the present embodiment, the first and second directions defined by the major axis Ix and the minor axis Iy of the image circle Is also do not need to be orthogonal to each other and may cross at various angles. Further, the lengths of the diameters of the image circle Is in the first and second directions may be the same. The image circle Is is not necessarily distorted from a circle.

In each of the above embodiments, the XY-polynomial surface and the anamorphic aspherical surface have been illustrated as an example of the freeform surface. In the present embodiment, the freeform surface is not limited to the above surface, and may be a toric surface, for example. Further, the imaging optical system of the present embodiment may include two or more freeform surfaces that are non-anamorphic on the object side of the diaphragm A. The non-anamorphic freeform surfaces include XY-polynomial surfaces but do not include anamorphic aspherical surfaces. The non-anamorphic freeform surface may have no symmetric plane, for example.

The imaging system 10 according to the present embodiment is applicable to various uses, for example, can be mounted in vehicles. For example, the imaging device 11 may constitute an in-vehicle camera for capturing an image of a scene behind a moving body such as a vehicle. Further, the imaging device 11 serving as an in-vehicle camera may be configured to capture not only a scene behind the moving body but also various scenes in front of the moving body or on the side of the moving body. Further, the imaging system 10 is not limited to be mounted in vehicles for use. For example, the imaging system 10 can be applied to a surveillance camera that monitors various situations or the like.

The embodiment has been described above as an illustration of the technique of the present disclosure. The accompanying drawings and the detailed description are provided for this purpose.

Therefore, components in the accompanying drawings and the detailed description may include not only components essential for solving problems, but also components that are not essential for solving the technical problems but are merely used to illustrate the technology disclosed herein. Therefore, such inessential components should not be readily construed as being essential based on the fact that such inessential components are shown in the accompanying drawings or mentioned in the detailed description.

Furthermore, since the embodiment described above is intended to illustrate the technique in the present disclosure, various changes, substitutions, additions, omissions, and the like can be made within the scope of the claims and the scope of equivalents thereof.

Summary of Aspects

Various aspects according to the present disclosure will be described below.

A first aspect according to the present disclosure provides an imaging optical system having an image circle formed on an imaging element. The imaging optical system includes a plurality of lens elements arranged from an object side to an image plane side, and a diaphragm arranged between the plurality of lens elements. The plurality of lens elements includes a freeform lens having a freeform surface that is asymmetrical between a first direction and a second direction which cross with each other. At least two freeform lenses are located on the object side of the diaphragm.

According to the imaging optical system described above, it is possible to facilitate to widen an angle of view in a specific direction by using the freeform surfaces of the plurality of freeform lenses located on the object side of the diaphragm.

In a second aspect, in the imaging optical system according to the first aspect, a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle. The imaging optical system satisfies a following conditional expression (1) based on a summation for the freeform surfaces of the freeform lenses located on the object side of the diaphragm.

[Equation  7] $\begin{matrix} {\frac{\sum\limits_{k = 1}^{N}\; {\left( {{SS}_{k} - {SL}_{k}} \right) \times \Delta \; {nd}_{k}}}{YSH} < 0} & (1) \end{matrix}$

where

N is a total number of freeform surfaces of the freeform lenses located on the object side of the diaphragm,

k is a number identifying a freeform surface among the total N freeform surfaces,

SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of the shortest image height,

SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height,

Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface, and

YSH is a height of 50% of the shortest image height. According to this configuration, the freeform surfaces located on the object side of the diaphragm in the imaging optical system can increase power negatively in the second direction rather than in the first direction as a whole, whereby an angle of view in the second direction can be widened.

In a third aspect, in the imaging optical system according to the first aspect, a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle. The imaging optical system satisfies a following conditional expression (2) based on a summation for the freeform surfaces of the freeform lenses located on the object side of the diaphragm.

[Equation  8] $\begin{matrix} {\frac{\sum\limits_{k = 1}^{N}\; {\left( {{SS}_{k} - {SL}_{k}} \right) \times \Delta \; {nd}_{k}}}{{CTL}\; 1} < {- 0.0002}} & (2) \end{matrix}$

where

N is a total number of freeform surfaces of the freeform lenses located on the object side of the diaphragm,

k is a number identifying a freeform surface among the total N freeform surfaces,

SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of the shortest image height,

SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height,

Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface, and

CTL1 is a thickness of a lens element located closest to the object side. This configuration makes it possible to suppress astigmatism and avoid an increase in size of the optical system for widening an angle of view in the second direction.

In a fourth aspect, in the imaging optical system according to the first aspect, a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle. The imaging optical system satisfies a following conditional expression (3) based on a summation for the freeform surfaces of the freeform lenses located on the object side of the diaphragm.

[Equation  9] $\begin{matrix} {\frac{\sum\limits_{k = 1}^{N}\; {\left( {{SS}_{k} - {SL}_{k}} \right) \times \Delta \; {nd}_{k}}}{CTF} < {- 0.001}} & (3) \end{matrix}$

where

N is a total number of freeform surfaces of the freeform lenses located on the object side of the diaphragm,

k is a number identifying a freeform surface among the total N freeform surfaces,

SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of the shortest image height,

SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height,

Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface, and

CTF is a thickness of a freeform lens located closest to the object side. This configuration can widen an angle of view in the second direction as well as avoiding an increase in size of the optical system.

In a fifth aspect, in the imaging optical system according to the first aspect, a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle. The imaging optical system satisfies a following conditional expression (4) based on a summation for both surfaces of a freeform lens located closest to the object side and a summation for both surfaces of a freeform lens located closest to the image plane side on the object side of the diaphragm.

[Equation  10] $\begin{matrix} {{- 2.00} < \frac{\sum\limits_{i = 1}^{2}\; {\left( {{SS}_{i} - {SL}_{i}} \right) \times \Delta \; {nd}_{i}}}{\sum\limits_{n = 1}^{2}\; {\left( {{SS}_{n} - {SL}_{n}} \right) \times \Delta \; {nd}_{n}}} < 3.00} & (4) \end{matrix}$

where,

i is a number identifying a surface of the freeform lens located closest to the object side,

SL_(i) is a sag amount at a position where a height of an i-th surface of the freeform lens located closest to the object side in the first direction is 50% of the shortest image height,

SS_(i) is a sag amount at a position where a height of the i-th surface in the second direction is 50% of the shortest image height,

Δnd_(i) is a difference resulting from subtracting a refractive index on the object side of the i-th surface from a refractive index on the image plane side of the i-th surface,

n is a number identifying a surface of the freeform lens located closest to the image plane side,

SL_(n) is a sag amount at a position where a height of an n-th surface of the freeform lens located closest to the image plane side in the first direction is 50% of the shortest image height,

SS_(n) is a sag amount at a position where a height of the n-th surface in the second direction is 50% of the shortest image height, and

Δnd_(n) is a difference resulting from subtracting a refractive index on the object side of the n-th surface from a refractive index on the image plane side of the n-th surface. According to this, astigmatism can be controlled well, and an angle of view in the second direction can be widened.

In a sixth aspect, in the imaging optical system according to the first aspect, a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle. The imaging optical system satisfies a following conditional expression (5).

[Equation  11] $\begin{matrix} {{- 8.00} < \frac{\left( {{SS}_{1} - {SL}_{1}} \right) \times \Delta \; {nd}_{1}}{\left( {{SS}_{N} - {SL}_{N}} \right) \times \Delta \; {nd}_{N}} < 0.00} & (5) \end{matrix}$

where

SL₁ is a sag amount at a position where a height of a freeform surface located closest to the object side in the first direction is 50% of the shortest image height,

SS₁ is a sag amount at a position where a height of the freeform surface located closest to the object side in the second direction is 50% of the shortest image height,

Δnd₁ is a difference resulting from subtracting a refractive index on the object side of the freeform surface located closest to the object side from a refractive index on the image plane side of the same freeform surface,

SL_(N) is a sag amount at a position where a height of a freeform surface located closest to the image plane side on the object side of the diaphragm in the first direction is 50% of the shortest image height,

SS_(N) is a sag amount at a position where a height of the freeform surface located closest to the image plane side in the second direction is 50% of the shortest image height, and

Δnd_(N) is a difference resulting from subtracting a refractive index on the object side of the freeform surface located closest to the image plane side from a refractive index on the image plane side of the same freeform surface. This configuration can widen an angle of view in the second direction as well as downsizing the optical system.

In a seventh aspect, the imaging optical system according to the first aspect satisfies a following conditional expression (6).

1≤nd1/ndN<1.3  (6)

where

nd1 is a refractive index to a d-line of a freeform lens located closest to the object side, and

ndN is a refractive index to the d-line of a freeform lens located closest to the image plane side on the object side of the diaphragm. This configuration makes it possible to widen an angle of view in the second direction as well as avoiding a situation in which it is difficult to control astigmatism and lateral chromatic aberration.

In an eighth aspect, the imaging optical system according to the first aspect satisfies a following conditional expression (7).

1.45<ndN<1.80  (7)

where ndN is a refractive index to a d-line of a freeform lens located closest to the image plane side on the object side of the diaphragm. This configuration makes it possible to widen an angle of view in the second direction as well as avoiding a situation in which it is difficult to control curvature of field and lateral chromatic aberration.

In a ninth aspect, in the imaging optical system according to the first aspect, the freeform lenses located on the object side of the diaphragm are adjacent to each other. This configuration makes it easier to control the action of an asymmetric component of a light flux, and can improve an asymmetric component of curvature of field.

In a tenth aspect, in the imaging optical system according to the first aspect, the plurality of lens elements includes a freeform lens located on the image plane side of the diaphragm. This configuration makes it easier to control resolution, such as to increase the resolution near the center of the image plane.

In an eleventh aspect, in the imaging optical system according to the first aspect, a lens element located closest to the object side is rotationally symmetrical with reference to an optical axis. According to this configuration, a manufacturing process of the imaging optical system can be simplified.

In a twelfth aspect, in the imaging optical system according to the first aspect, all freeform surfaces of the freeform lenses located on the object side of the diaphragm have a same sign of (SS_(k)−SL_(k)), where

k is a number identifying a freeform surface among the freeform surfaces of the freeform lenses located on the object side of the diaphragm,

SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of the shortest image height,

SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height, and

Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface. This configuration can gradually bend entering light beam to thereby suppress an occurrence of aberration, for widening an angle of view in the second direction on the freeform surfaces located on the object side of the diaphragm.

A thirteenth aspect provides an imaging device including the imaging optical system according to any one of the first to twelfth aspects and an imaging element. The imaging element captures an image formed by the imaging optical system. The imaging element has a first side which corresponds to the first direction and a second side which corresponds to the second direction and has a length equal to or shorter than the first side. The imaging optical system can easily widen an angle of view of the imaging device in a specific direction.

A fourteenth aspect provides an imaging system including the imaging device according to the thirteenth aspect and an image processor. The image processor performs image processing on the image captured by the imaging element of the imaging device. The imaging optical system can easily widen an angle of view of the imaging system in a specific direction.

INDUSTRIAL APPLICABILITY

The imaging system according to the present disclosure is applicable to various uses for capturing images, such as an in-vehicle camera, a surveillance camera, a web camera, a digital camera, and the like. Further, the imaging optical system according to the present disclosure may be provided in an interchangeable lens device. 

1. An imaging optical system having an image circle formed on an imaging element, the imaging optical system comprising: a plurality of lens elements arranged from an object side to an image plane side, and a diaphragm arranged between the plurality of lens elements, wherein the plurality of lens elements includes a freeform lens having a freeform surface that is asymmetrical with respect to a first direction and a second direction which cross with each other, wherein at least two freeform lenses are located on the object side of the diaphragm.
 2. The imaging optical system according to claim 1, wherein a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle, wherein the imaging optical system satisfies a following conditional expression (1) based on a summation for freeform surfaces of freeform lenses located on the object side of the diaphragm: [Equation  1] $\begin{matrix} {\frac{\sum\limits_{k = 1}^{N}\; {\left( {{SS}_{k} - {SL}_{k}} \right) \times \Delta \; {nd}_{k}}}{YSH} < 0} & (1) \end{matrix}$ where N is a total number of the freeform surfaces of the freeform lenses located on the object side of the diaphragm, k is a number identifying a freeform surface among the total N freeform surfaces, SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of shortest image height, SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height, Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface, and YSH is a height of 50% of the shortest image height.
 3. The imaging optical system according to claim 1, wherein a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle, wherein the imaging optical system satisfies a following conditional expression (2) based on a summation for freeform surfaces of freeform lenses located on the object side of the diaphragm: [Equation  2] $\begin{matrix} {\frac{\sum\limits_{k = 1}^{N}\; {\left( {{SS}_{k} - {SL}_{k}} \right) \times \Delta \; {nd}_{k}}}{{CTL}\; 1} < {- 0.0002}} & (2) \end{matrix}$ where N is a total number of the freeform surfaces of the freeform lenses located on the object side of the diaphragm, k is a number identifying a freeform surface among the total N freeform surfaces, SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of shortest image height, SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height, Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface, and CTL1 is a thickness of a lens element located closest to the object side.
 4. The imaging optical system according to claim 1, wherein a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle, wherein the imaging optical system satisfies a following conditional expression (3) based on a summation for the freeform surfaces of freeform lenses located on the object side of the diaphragm: [Equation  3] $\begin{matrix} {\frac{\sum\limits_{k = 1}^{N}\; {\left( {{SS}_{k} - {SL}_{k}} \right) \times \Delta \; {nd}_{k}}}{CTF} < {- 0.001}} & (3) \end{matrix}$ where N is a total number of the freeform surfaces of the freeform lenses located on the object side of the diaphragm, k is a number identifying a freeform surface among the total N freeform surfaces, SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of shortest image height, SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height, Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface, and CTF is a thickness of a freeform lens located closest to the object side.
 5. The imaging optical system according to claim 1, wherein a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle, wherein the imaging optical system satisfies a following conditional expression (4) based on a summation for both surfaces of a freeform lens located closest to the object side and a summation for both surfaces of a freeform lens located closest to the image plane side on the object side of the diaphragm: [Equation  4] $\begin{matrix} {{- 2.00} < \frac{\sum\limits_{i = 1}^{2}\; {\left( {{SS}_{i} - {SL}_{i}} \right) \times \Delta \; {nd}_{i}}}{\sum\limits_{n = 1}^{2}\; {\left( {{SS}_{n} - {SL}_{n}} \right) \times \Delta \; {nd}_{n}}} < 3.00} & (4) \end{matrix}$ where i is a number identifying a surface of the freeform lens located closest to the object side, SL_(i) is a sag amount at a position where a height of an i-th surface of the freeform lens located closest to the object side in the first direction is 50% of shortest image height, SS_(i) is a sag amount at a position where a height of the i-th surface in the second direction is 50% of the shortest image height, Δnd_(i) is a difference resulting from subtracting a refractive index on the object side of the i-th surface from a refractive index on the image plane side of the i-th surface, n is a number identifying a surface of the freeform lens located closest to the image plane side, SL_(n) is a sag amount at a position where a height of an n-th surface of the freeform lens located closest to the image plane side in the first direction is 50% of the shortest image height, SS_(n) is a sag amount at a position where a height of the n-th surface in the second direction is 50% of the shortest image height, and Δnd_(n) is a difference resulting from subtracting a refractive index on the object side of the n-th surface from a refractive index on the image plane side of the n-th surface.
 6. The imaging optical system according to claim 1, wherein a diameter in the first direction is equal to or larger than a diameter in the second direction in the image circle, wherein the imaging optical system satisfies a following conditional expression (5): [Equation  5] $\begin{matrix} {{- 8.00} < \frac{\left( {{SS}_{1} - {SL}_{1}} \right) \times \Delta \; {nd}_{1}}{\left( {{SS}_{N} - {SL}_{N}} \right) \times \Delta \; {nd}_{N}} < 0.00} & (5) \end{matrix}$ where SL₁ is a sag amount at a position where a height of a freeform surface located closest to the object side in the first direction is 50% of shortest image height, SS₁ is a sag amount at a position where a height of the freeform surface located closest to the object side in the second direction is 50% of the shortest image height, Δnd₁ is a difference resulting from subtracting a refractive index on the object side of the freeform surface located closest to the object side from a refractive index on the image plane side of the same freeform surface, SL_(N) is a sag amount at a position where a height of a freeform surface located closest to the image plane side on the object side of the diaphragm in the first direction is 50% of the shortest image height, SS_(N) is a sag amount at a position where a height of the freeform surface located closest to the image plane side in the second direction is 50% of the shortest image height, and Δnd_(N) is a difference resulting from subtracting a refractive index on the object side of the freeform surface located closest to the image plane side from a refractive index on the image plane side of the same freeform surface.
 7. The imaging optical system according to claim 1, satisfying a following conditional expression (6): 1≤nd1/ndN<1.3  (6) where nd1 is a refractive index to a d-line of a freeform lens located closest to the object side, and ndN is a refractive index to the d-line of a freeform lens located closest to the image plane side on the object side of the diaphragm.
 8. The imaging optical system according to claim 1, satisfying a following conditional expression (7): 1.45<ndN<1.80  (7) where ndN is a refractive index to a d-line of a freeform lens located closest to the image plane side on the object side of the diaphragm.
 9. The imaging optical system according to claim 1, wherein freeform lenses located on the object side of the diaphragm are adjacent to each other.
 10. The imaging optical system according to claim 1, wherein the plurality of lens elements includes a freeform lens located on the image plane side of the diaphragm.
 11. The imaging optical system according to claim 1, wherein a lens element located closest to the object side is rotationally symmetrical with reference to an optical axis.
 12. The imaging optical system according to claim 1, wherein all freeform surfaces of the freeform lenses located on the object side of the diaphragm have a same sign of (SS_(k)−SL_(k)), where k is a number identifying a freeform surface among the freeform surfaces of the freeform lenses located on the object side of the diaphragm, SL_(k) is a sag amount at a position where a height of a k-th freeform surface in the first direction is 50% of shortest image height, SS_(k) is a sag amount at a position where a height of the k-th freeform surface in the second direction is 50% of the shortest image height, and Δnd_(k) is a difference resulting from subtracting a refractive index on the object side of the k-th freeform surface from a refractive index on the image plane side of the k-th freeform surface.
 13. An imaging device comprising: the imaging optical system according to claim 1, and an imaging element to capture an image formed by the imaging optical system, wherein the imaging element has a first side which corresponds to the first direction and a second side which corresponds to the second direction and has a length equal to or shorter than the first side.
 14. An imaging system comprising: the imaging device according to claim 13, and an image processor to perform image processing on the image captured by the imaging element of the imaging device. 